Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807020272/lh2370sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807020272/lh2370Isup2.hkl |
CCDC reference: 647722
The title compound (I) was prepared by reacting diformylhydrazine (0.046 mol, 4.0 g) and 3-amino-1,2,4-triazole 0.046 mol,3.9 g). The reactant mixture was heated slowly to 433 K for an hour. The cooled reaction mixture was dissolved in 25 ml of boiling water and filtered. On cooling, 4.4 g of the product separated. Recrystallization from hot water gave large white crystals. Elemental analysis(%) for C4H6N6O, found (calculated): C 31.12 (31.13), H 3.80 (3.89), N 54.60 (54.49). IR(cm-1,KBr):3352.21, 3119.57,2881.59, 2733.65,1789.84,1657.08,1575.38,1505.81,1371.08,1303.73, 1290.26,1142.12, 1051.33,986.29, 958.04,897.31,877.09,738.58, 629.96,563.66.
When the structure of (I) is solved and refined in the centrosymmtric space group C2/c with half a molecule in the asymmetric unit, the structure is disordered with R values that are significantly higher (R1=15 and wR2=34%) and the anistropic displacement parameters have unusual values. In the absence of significant anomalous dispersion effects Friedel pairs were merged. H atoms bonded to O1 and N1 were located from the difference maps with and refined with constraints of O–H = 0.86 (2) Å, H–H =1.35 (2) Å, N–H = 0.86 (2) Å; Uiso(H) = 1.5Ueq(O) and Uiso(H) = 1.2Ueq(N). H2, H3 and H4 were placed in calculated positions with C—H = 0.93 Å and Uiso(H) =1.2Ueq(C).
Recent interest in substituted 1,2,4-triazoles has arisen in part from their transition metal complexes with intriguing structures and specific magnetic properties (Garcia et al.,1997; Kahn & Martinez,1998; Fujigaya et al.,2003). However bitriazole ligands have not been extensively exploited up to now, and herein we reported the crystal structure of (I).
In (I) (Fig.2), the two triazole ring are almost coplanar with a dihedral angle of 2.97 (1)° between them. The bond lengths and angles are unremarkable.
The crystal structure is stablized by one N–H···O, two O–H···N and three C–H···N(or O) hydrogen bonds. In detail, the water O atom O1 acts as a hydrogen bond donor, via. H1A and H1B, to the atom N5 at (-3/2 + x, 1/2 - y, -1/2 + z) and atom N6 (x, 1/2 + y, z), respectively, forming a one-dimensional chain along the [001] direction. In addition, the atom N2 at (x,y,z) acts as hydrogen bond donor, via. H2A, to the water O atom O1 in the same symmetric unit, linking adjacent chains into a three dimensional framework (Fig.3). Analysis using PLATON (Spek, 2003) shows that there are other three C–H···N(or O)(Table 2) hydrogen bonds which further stabilize the crystal structure. In addtion, π–π interactions are observed between the triazole ring N1—N3/C1/C2 at (x, y, z) and the other five-numbered ring N4—N6/C3/C4 at (-1 + x, y, z). The dihedral angle between the two triazole rings is only 2.97 (1)°, with an interplanar spacing of 3.273 (1) Å, a ring centroid separation of 3.635 (1) Å.
There has been recent interest in substituted 1,2,4-triazoles (Fujigaya et al., 2003; Garcia et al., 1997; Kahn & Martinez, 1998).
Data collection: SMART (Bruker, 2001); cell refinement: SAINT-Plus (Bruker, 2001); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: PLATON.
C4H4N6·H2O | F(000) = 320 |
Mr = 154.15 | Dx = 1.538 Mg m−3 |
Monoclinic, Cc | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: C -2yc | Cell parameters from 1837 reflections |
a = 3.8716 (3) Å | θ = 2.6–28.1° |
b = 15.8019 (14) Å | µ = 0.12 mm−1 |
c = 10.8874 (9) Å | T = 296 K |
β = 91.785 (1)° | Plate, colorless |
V = 665.75 (10) Å3 | 0.20 × 0.10 × 0.04 mm |
Z = 4 |
Bruker SMART APEX CCD area-detector diffractometer | 727 independent reflections |
Radiation source: fine focus sealed Siemens Mo tube | 709 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.027 |
0.3° wide ω exposures scans | θmax = 27.0°, θmin = 2.6° |
Absorption correction: multi-scan (SADABS; Sheldrick, 2001) | h = −4→4 |
Tmin = 0.976, Tmax = 0.988 | k = −18→20 |
2254 measured reflections | l = −13→13 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.034 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.089 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.06 | w = 1/[σ2(Fo2) + (0.0579P)2 + 0.1815P] where P = (Fo2 + 2Fc2)/3 |
727 reflections | (Δ/σ)max < 0.001 |
110 parameters | Δρmax = 0.17 e Å−3 |
6 restraints | Δρmin = −0.21 e Å−3 |
C4H4N6·H2O | V = 665.75 (10) Å3 |
Mr = 154.15 | Z = 4 |
Monoclinic, Cc | Mo Kα radiation |
a = 3.8716 (3) Å | µ = 0.12 mm−1 |
b = 15.8019 (14) Å | T = 296 K |
c = 10.8874 (9) Å | 0.20 × 0.10 × 0.04 mm |
β = 91.785 (1)° |
Bruker SMART APEX CCD area-detector diffractometer | 727 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2001) | 709 reflections with I > 2σ(I) |
Tmin = 0.976, Tmax = 0.988 | Rint = 0.027 |
2254 measured reflections |
R[F2 > 2σ(F2)] = 0.034 | 6 restraints |
wR(F2) = 0.089 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.06 | Δρmax = 0.17 e Å−3 |
727 reflections | Δρmin = −0.21 e Å−3 |
110 parameters |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.1950 (6) | 0.28332 (13) | 0.7395 (2) | 0.0286 (5) | |
C2 | −0.0527 (8) | 0.39041 (17) | 0.7999 (2) | 0.0403 (6) | |
H2 | −0.1431 | 0.4331 | 0.8481 | 0.048* | |
C3 | 0.4923 (7) | 0.16139 (17) | 0.6439 (2) | 0.0383 (6) | |
H3 | 0.4433 | 0.1745 | 0.5619 | 0.046* | |
C4 | 0.5157 (8) | 0.16590 (16) | 0.8413 (2) | 0.0363 (6) | |
H4 | 0.4867 | 0.1829 | 0.9222 | 0.044* | |
N1 | 0.0761 (6) | 0.31653 (13) | 0.63646 (19) | 0.0363 (5) | |
N2 | −0.0840 (6) | 0.38719 (14) | 0.67866 (19) | 0.0378 (5) | |
H2A | −0.187 (8) | 0.4237 (18) | 0.627 (3) | 0.052 (9)* | |
N3 | 0.1248 (7) | 0.32463 (13) | 0.84350 (19) | 0.0385 (6) | |
N4 | 0.3879 (5) | 0.20801 (11) | 0.74086 (18) | 0.0293 (4) | |
N5 | 0.6829 (6) | 0.09913 (14) | 0.80910 (18) | 0.0406 (6) | |
N6 | 0.6694 (7) | 0.09619 (14) | 0.6813 (2) | 0.0412 (5) | |
O1 | −0.4451 (6) | 0.48966 (11) | 0.5130 (2) | 0.0423 (5) | |
H1A | −0.584 (9) | 0.465 (2) | 0.466 (3) | 0.064* | |
H1B | −0.561 (9) | 0.5245 (19) | 0.553 (3) | 0.064* |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0330 (12) | 0.0295 (9) | 0.0236 (9) | −0.0055 (8) | 0.0036 (8) | 0.0001 (8) |
C2 | 0.0498 (16) | 0.0358 (12) | 0.0356 (13) | 0.0012 (10) | 0.0075 (11) | −0.0059 (10) |
C3 | 0.0481 (16) | 0.0390 (12) | 0.0278 (11) | 0.0028 (10) | 0.0025 (11) | −0.0035 (9) |
C4 | 0.0460 (14) | 0.0405 (12) | 0.0224 (10) | −0.0007 (10) | −0.0013 (10) | 0.0025 (9) |
N1 | 0.0455 (13) | 0.0365 (11) | 0.0268 (9) | 0.0037 (8) | 0.0011 (8) | 0.0003 (7) |
N2 | 0.0440 (13) | 0.0332 (10) | 0.0363 (10) | 0.0019 (8) | 0.0039 (9) | 0.0028 (8) |
N3 | 0.0513 (14) | 0.0393 (11) | 0.0251 (9) | 0.0028 (9) | 0.0041 (9) | −0.0040 (7) |
N4 | 0.0346 (11) | 0.0325 (9) | 0.0208 (7) | −0.0021 (7) | 0.0011 (7) | −0.0002 (7) |
N5 | 0.0477 (15) | 0.0401 (12) | 0.0336 (11) | 0.0011 (9) | −0.0034 (9) | 0.0049 (8) |
N6 | 0.0472 (14) | 0.0390 (12) | 0.0373 (11) | 0.0036 (10) | 0.0030 (10) | −0.0022 (9) |
O1 | 0.0460 (10) | 0.0415 (10) | 0.0393 (11) | 0.0033 (9) | −0.0030 (8) | −0.0040 (7) |
C1—N1 | 1.309 (3) | C4—N5 | 1.292 (4) |
C1—N3 | 1.342 (3) | C4—N4 | 1.360 (3) |
C1—N4 | 1.405 (3) | C4—H4 | 0.9300 |
C2—N2 | 1.323 (3) | N1—N2 | 1.364 (3) |
C2—N3 | 1.326 (4) | N2—O1 | 2.770 (3) |
C2—H2 | 0.9300 | N2—H2A | 0.895 (18) |
C3—N6 | 1.296 (4) | N5—N6 | 1.392 (3) |
C3—N4 | 1.359 (3) | O1—H1A | 0.835 (18) |
C3—H3 | 0.9300 | O1—H1B | 0.840 (19) |
N1—C1—N3 | 116.9 (2) | C2—N2—O1 | 131.0 (2) |
N1—C1—N4 | 121.40 (19) | N1—N2—O1 | 119.00 (16) |
N3—C1—N4 | 121.67 (19) | C2—N2—H2A | 129 (2) |
N2—C2—N3 | 111.0 (3) | N1—N2—H2A | 121 (2) |
N2—C2—H2 | 124.5 | C2—N3—C1 | 101.3 (2) |
N3—C2—H2 | 124.5 | C3—N4—C4 | 104.5 (2) |
N6—C3—N4 | 110.7 (2) | C3—N4—C1 | 128.46 (19) |
N6—C3—H3 | 124.6 | C4—N4—C1 | 127.06 (19) |
N4—C3—H3 | 124.6 | C4—N5—N6 | 107.2 (2) |
N5—C4—N4 | 110.7 (2) | C3—N6—N5 | 106.9 (2) |
N5—C4—H4 | 124.6 | N2—O1—H1A | 115 (3) |
N4—C4—H4 | 124.6 | N2—O1—H1B | 108 (3) |
C1—N1—N2 | 101.0 (2) | H1A—O1—H1B | 107 (3) |
C2—N2—N1 | 109.8 (2) | ||
N3—C1—N1—N2 | 0.8 (3) | N6—C3—N4—C1 | 179.3 (2) |
N4—C1—N1—N2 | −179.09 (19) | N5—C4—N4—C3 | −0.2 (3) |
N3—C2—N2—N1 | 0.3 (3) | N5—C4—N4—C1 | −179.5 (2) |
N3—C2—N2—O1 | 175.2 (2) | N1—C1—N4—C3 | 3.1 (3) |
C1—N1—N2—C2 | −0.6 (3) | N3—C1—N4—C3 | −176.8 (3) |
C1—N1—N2—O1 | −176.24 (17) | N1—C1—N4—C4 | −177.7 (3) |
N2—C2—N3—C1 | 0.2 (3) | N3—C1—N4—C4 | 2.4 (3) |
N1—C1—N3—C2 | −0.6 (3) | N4—C4—N5—N6 | 0.3 (3) |
N4—C1—N3—C2 | 179.2 (2) | N4—C3—N6—N5 | 0.2 (3) |
N6—C3—N4—C4 | 0.0 (3) | C4—N5—N6—C3 | −0.4 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1A···N5i | 0.84 (2) | 2.15 (2) | 2.962 (3) | 163 (4) |
O1—H1B···N6ii | 0.84 (2) | 2.10 (2) | 2.930 (3) | 169 (4) |
C2—H2···O1iii | 0.93 | 2.49 | 3.392 (3) | 163 |
C3—H3···N3iv | 0.93 | 2.50 | 3.334 (3) | 149 |
C4—H4···N1v | 0.93 | 2.35 | 3.226 (3) | 157 |
N2—H2A···O1 | 0.90 (2) | 1.88 (2) | 2.770 (3) | 173 (3) |
Symmetry codes: (i) x−3/2, −y+1/2, z−1/2; (ii) x−3/2, y+1/2, z; (iii) x, −y+1, z+1/2; (iv) x+1/2, −y+1/2, z−1/2; (v) x+1/2, −y+1/2, z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C4H4N6·H2O |
Mr | 154.15 |
Crystal system, space group | Monoclinic, Cc |
Temperature (K) | 296 |
a, b, c (Å) | 3.8716 (3), 15.8019 (14), 10.8874 (9) |
β (°) | 91.785 (1) |
V (Å3) | 665.75 (10) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.12 |
Crystal size (mm) | 0.20 × 0.10 × 0.04 |
Data collection | |
Diffractometer | Bruker SMART APEX CCD area-detector |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2001) |
Tmin, Tmax | 0.976, 0.988 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 2254, 727, 709 |
Rint | 0.027 |
(sin θ/λ)max (Å−1) | 0.639 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.034, 0.089, 1.06 |
No. of reflections | 727 |
No. of parameters | 110 |
No. of restraints | 6 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.17, −0.21 |
Computer programs: SMART (Bruker, 2001), SAINT-Plus (Bruker, 2001), SAINT-Plus, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2003), PLATON.
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1A···N5i | 0.835 (18) | 2.15 (2) | 2.962 (3) | 163 (4) |
O1—H1B···N6ii | 0.840 (19) | 2.10 (2) | 2.930 (3) | 169 (4) |
C2—H2···O1iii | 0.93 | 2.49 | 3.392 (3) | 162.8 |
C3—H3···N3iv | 0.93 | 2.50 | 3.334 (3) | 149.2 |
C4—H4···N1v | 0.93 | 2.35 | 3.226 (3) | 157.4 |
N2—H2A···O1 | 0.895 (18) | 1.879 (19) | 2.770 (3) | 173 (3) |
Symmetry codes: (i) x−3/2, −y+1/2, z−1/2; (ii) x−3/2, y+1/2, z; (iii) x, −y+1, z+1/2; (iv) x+1/2, −y+1/2, z−1/2; (v) x+1/2, −y+1/2, z+1/2. |
Recent interest in substituted 1,2,4-triazoles has arisen in part from their transition metal complexes with intriguing structures and specific magnetic properties (Garcia et al.,1997; Kahn & Martinez,1998; Fujigaya et al.,2003). However bitriazole ligands have not been extensively exploited up to now, and herein we reported the crystal structure of (I).
In (I) (Fig.2), the two triazole ring are almost coplanar with a dihedral angle of 2.97 (1)° between them. The bond lengths and angles are unremarkable.
The crystal structure is stablized by one N–H···O, two O–H···N and three C–H···N(or O) hydrogen bonds. In detail, the water O atom O1 acts as a hydrogen bond donor, via. H1A and H1B, to the atom N5 at (-3/2 + x, 1/2 - y, -1/2 + z) and atom N6 (x, 1/2 + y, z), respectively, forming a one-dimensional chain along the [001] direction. In addition, the atom N2 at (x,y,z) acts as hydrogen bond donor, via. H2A, to the water O atom O1 in the same symmetric unit, linking adjacent chains into a three dimensional framework (Fig.3). Analysis using PLATON (Spek, 2003) shows that there are other three C–H···N(or O)(Table 2) hydrogen bonds which further stabilize the crystal structure. In addtion, π–π interactions are observed between the triazole ring N1—N3/C1/C2 at (x, y, z) and the other five-numbered ring N4—N6/C3/C4 at (-1 + x, y, z). The dihedral angle between the two triazole rings is only 2.97 (1)°, with an interplanar spacing of 3.273 (1) Å, a ring centroid separation of 3.635 (1) Å.